2943 - 2946 |
Long-range charge-transfer excited states in time-dependent density functional theory require non-local exchange Dreuw A, Weisman JL, Head-Gordon M |
2947 - 2950 |
IR induced cis <-> trans isomerization of 2-naphthol: Catalytic role of hydrogen-bond in the photoinduced isomerization Ebata T, Kouyama K, Mikami N |
2951 - 2962 |
Method of moments of coupled-cluster equations: The quasivariational and quadratic approximations Pimienta ISO, Kowalski K, Piecuch P |
2963 - 2971 |
The generalized active space concept for the relativistic treatment of electron correlation. II. Large-scale configuration interaction implementation based on relativistic 2- and 4-spinors and its application Fleig T, Olsen J, Visscher L |
2972 - 2977 |
A real-space model of nondynamical correlation Becke AD |
2978 - 2990 |
Density-functional theory calculations with correct long-range potentials Wu Q, Ayers PW, Yang WT |
2991 - 3004 |
Analytic first derivatives for general coupled-cluster and configuration interaction models Kallay M, Gauss J, Szalay PG |
3005 - 3014 |
The role of the basis set: Assessing density functional theory Boese AD, Martin JML, Handy NC |
3015 - 3024 |
The exchange-correlation potential in Kohn-Sham nuclear magnetic resonance shielding calculations Keal TW, Tozer DJ |
3025 - 3039 |
Modeling induced polarization with classical Drude oscillators: Theory and molecular dynamics simulation algorithm Lamoureux G, Roux B |
3040 - 3050 |
Direct dynamics study of energy transfer and collision-induced dissociation: Effects of impact energy, geometry, and reactant vibrational mode in H2CO+-Ne collisions Liu JB, Song K, Hase WL, Anderson SL |
3051 - 3062 |
Charge transfer effects in molecule-negative ion complexes induced by core ionization Streltsov AI, Dobrodey NV, Cederbaum LS |
3063 - 3070 |
Implementation of a fast analytic ground state potential energy surface for the N(D-2)+H-2 reaction Ho TS, Rabitz H, Aoiz FJ, Banares L, Vazquez SA, Harding LB |
3071 - 3077 |
Anion clusters of anthracene, An(n)(-) (n=1-16) Song JK, Lee NK, Kim JH, Han SY, Kim SK |
3078 - 3084 |
Time averaging the semiclassical initial value representation for the calculation of vibrational energy levels. II. Application to H2CO, NH3, CH4, CH2D2 Kaledin AL, Miller WH |
3085 - 3091 |
The role of phase in molecular Rydberg wave packet dynamics Smith RAL, Stavros VG, Verlet JRR, Fielding HH, Townsend D, Softley TP |
3092 - 3097 |
The vibrational spectrum of cyclic ozone Siebert R, Schinke R |
3098 - 3105 |
A variational study of nuclear dynamics and structural flexibility of the CH2OH radical Marenich AV, Boggs JE |
3106 - 3119 |
Benchmark theoretical study of the ionization threshold of benzene and oligoacenes Deleuze MS, Claes L, Kryachko ES, Francois JP |
3120 - 3129 |
Ab initio study of nonhomogeneous broadening of the zero-field splitting of triplet guest molecules in diluted glasses Loboda O, Minaev B, Vahtras O, Ruud K, Agren H |
3130 - 3137 |
Bound state properties and astrophysical applications of negatively charged hydrogen ions Frolov AM, Smith VH |
3138 - 3147 |
Homogeneous nucleation rates for D2O in a supersonic Laval nozzle Khan A, Heath CH, Dieregsweiler UM, Wyslouzil BE, Strey R |
3148 - 3159 |
Double-valued potential energy surface for H2O derived from accurate ab initio data and including long-range interactions Brandao J, Rio CMA |
3160 - 3173 |
Extreme ultraviolet laser excitation of isotopic molecular nitrogen: The dipole-allowed spectrum of N-15(2) and (NN)-N-14-N-15 Sprengers JP, Ubachs W, Baldwin KGH, Lewis BR, Tchang-Brillet WUL |
3174 - 3186 |
Velocity redistribution of excited atoms by radiative excitation transfer. I. Experimental demonstration by photodissociation of Na-2 and field-free imaging Kaufmann O, Ekers A, Bergmann K, Bezuglov N, Miculis K, Auzinsh M, Meyer W |
3187 - 3207 |
Accurate analytic He-H-2 potential energy surface from a greatly expanded set of ab initio energies Boothroyd AI, Martin PG, Peterson MR |
3208 - 3218 |
Theoretical investigation of weak hydrogen bonds to sulfur Wennmohs F, Staemmler V, Schindler M |
3219 - 3233 |
High resolution absorption spectrum of jet-cooled OCS between 64000 and 91000 cm-1 Cossart-Magos C, Jungen M, Xu R, Launay F |
3234 - 3239 |
Rotational and hyperfine analysis of the near infrared (3)Phi(4)-X-3 Phi(4) transitions of CoCl and CoI Wong AL, Tam WS, Cheung ASC |
3240 - 3248 |
Modelling the bacterial photosynthetic reaction center. V. Assignment of the electronic transition observed at 2200 cm(-1) in the special-pair radical-cation as a second-highest occupied molecular orbital to highest occupied molecular orbital transition Reimers JR, Shapley WA, Hush NS |
3249 - 3261 |
Modelling the bacterial photosynthetic reaction center. VI. Use of density-functional theory to determine the nature of the vibronic coupling between the four lowest-energy electronic states of the special-pair radical cation Reimers JR, Shapley WA, Rendell AP, Hush NS |
3262 - 3277 |
Modeling the bacterial photosynthetic reaction center. VII. Full simulation of the intervalence hole-transfer absorption spectrum of the special-pair radical cation Reimers JR, Hush NS |
3278 - 3290 |
Simulation and theory of vibrational phase relaxation in the critical and supercritical nitrogen: Origin of observed anomalies Roychowdhury S, Bagchi B |
3291 - 3296 |
Microscopic fluctuations and pattern formation in a supercritical oscillatory chemical system Hastings HM, Field RJ, Sobel SG |
3297 - 3308 |
Chemical-shift gamma-encoding nuclear magnetic resonance for uniaxially oriented matter under sample spinning Nishiyama Y, Kubo A, Terao T |
3309 - 3315 |
Critical-point and coexistence curve properties of a symmetric mixture of nonadditive hard spheres: A finite size scaling study Gozdz WT |
3316 - 3319 |
Fast time-resolved spectroscopy in shock compressed matter Holmes NC, Chau R |
3320 - 3331 |
A multimode vibronic treatment of absorption, resonance Raman, and hyper-Rayleigh scattering of excitonically coupled molecular dimers Kelley AM |
3332 - 3335 |
Defect hydrogen vibrations in various phases deuterium ice Li JC, Wang Y, Dong SL, Zhang P, Kolesnikov AI |
3336 - 3342 |
Microcanonical thermodynamic properties of helium nanodroplets Lehmann KK |
3343 - 3346 |
Molecular dynamics simulation of anomalous self-diffusion for single-file fluids Mon KK, Percus JK |
3347 - 3353 |
Neutron diffraction studies on aqueous solutions of glucose Mason PE, Neilson GW, Barnes AC, Enderby JE, Brady JW, Saboungi ML |
3354 - 3359 |
The effect of the order of autocatalysis for reaction fronts in vertical slabs Coroian DI, Vasquez DA |
3360 - 3370 |
Phenomenology of colloidal crystal electrophoresis Medebach M, Palberg T |
3371 - 3383 |
A real-space analysis of colloidal crystallization in a gravitational field at a flat bottom wall Hoogenboom JP, Vergeer P, van Blaaderen A |
3384 - 3390 |
Raman spectroscopy of template grown single wall carbon nanotubes in zeolite crystals Hulman M, Kuzmany H, Dubay O, Kresse G, Li L, Tang ZK |
3391 - 3404 |
Kinetic Monte Carlo simulation of the effect of coalescence energy release on the size and shape evolution of nanoparticles grown as an aerosol Mukherjee D, Sonwane CG, Zachariah MR |
3405 - 3412 |
Surface tension and vapor-liquid phase coexistence of the square-well fluid Singh JK, Kofke DA, Errington JR |
3413 - 3420 |
Energy transfer in collisions of peptide ions with surfaces Laskin J, Futrell JH |
3421 - 3428 |
Effects of molecular distribution on the fluorescence transfer: Exact results for slab geometry Klushin L, Tcherkasskaya O |
3429 - 3435 |
Thermal stability and partial dewetting of crystalline organic thin films: 3,4,9,10-perylenetetracarboxylic dianhydride on Ag(111) Krause B, Durr AC, Schreiber F, Dosch H, Seeck OH |
3436 - 3440 |
Elastic deformation of helical-conical boron nitride nanotubes Xu FF, Bando Y, Golberg D, Ma RZ, Li YB, Tang CC |
3441 - 3452 |
Partition thermodynamics of ionic surfactants between phosphatidylcholine vesicle and water phases Chu SC, Hung CH, Wang SC, Tsao HK |
3453 - 3460 |
Three-dimensional functional model proteins: Structure function and evolution Blackburne BP, Hirst JD |
3461 - 3467 |
Reorientation dynamics in a nematic liquid crystal studied by fast field cycling nuclear magnetic resonance Acosta RH, Pusiol DJ |
3468 - 3482 |
H-1 multiple-quantum nuclear magnetic resonance investigations of molecular order distributions in poly(dimethylsiloxane) networks: Evidence for a linear mixing law in bimodal systems Saalwachter K, Ziegler P, Spyckerelle O, Haidar B, Vidal A, Sommer JU |
3483 - 3494 |
Free energy formalism for polymer adsorption: Self-consistent field theory for weak adsorption Blokhuis EM, Skau KI, Avalos JB |
3495 - 3500 |
Hard sphere fluids in random fiber networks Schmidt M, Brader JM |
3501 - 3508 |
Power law kinetics in reversible enzyme-catalyzed reaction due to diffusion Paul S, Gangopadhyay G |
3509 - 3515 |
Computer simulations of a liquid crystalline dendrimer in liquid crystalline solvents Wilson MR, Ilnytskyi JM, Stimson LM |
3516 - 3528 |
Computing the electrostatic free-energy of complex molecules: The variational Coulomb field approximation Borgis D, Levy N, Marchi M |
3529 - 3534 |
Effect of particle size and shape on the order-disorder phase transition in diblock copolymers Chervanyov AI, Balazs AC |
3535 - 3540 |
Isotropic-nematic transition of long, thin, hard spherocylinders confined in a quasi-two-dimensional planar geometry Lagomarsino MC, Dogterom M, Dijkstra M |
3541 - 3549 |
Swelling behavior of responsive amphiphilic gels Jarkova E, Lee NK, Vilgis TA |
3550 - 3558 |
Multiple versus single pathways in electron transfer in proteins: Influence of protein dynamics and hydrogen bonds Kobayashi C, Baldridge K, Onuchic JN |
3559 - 3566 |
Free energy calculation from steered molecular dynamics simulations using Jarzynski's equality Park S, Khalili-Araghi F, Tajkhorshid E, Schulten K |
3567 - 3573 |
Helical twisting power and scaled chiral indices Neal MP, Solymosi M, Wilson MR, Earl DJ |
3574 - 3581 |
Effects of charge-charge interactions on dimensions of unfolded proteins: A Monte Carlo study Kundrotas PJ, Karshikoff A |